Lorentz vs space time interval

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Discussion Overview

The discussion revolves around the relationship between the Lorentz transformation and the invariance of the space-time interval in the context of special relativity. Participants explore how to calculate the time interval measured in a moving frame (S') between two events that occur simultaneously in a stationary frame (S), as well as the implications of length contraction and simultaneity.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant presents a calculation using the Lorentz transform to find the time interval t' between two events, leading to a result that includes the Lorentz factor gamma.
  • Another participant points out an inconsistency in the calculations related to the use of the space-time interval and the transformation of coordinates, suggesting that the participant misapplied the relationship between x and x'.
  • A third participant expresses confusion regarding the relationship between the lengths measured in different frames, questioning why x' should be less than x due to length contraction.
  • One participant clarifies that events simultaneous in one frame are not necessarily simultaneous in another, which affects the interpretation of length contraction.
  • Another participant acknowledges their misunderstanding and seeks further clarification on how to derive t' without using the Lorentz transformations, indicating a desire to explore the topic further.

Areas of Agreement / Disagreement

Participants express differing views on the implications of length contraction and simultaneity, with some clarifying misconceptions while others remain uncertain about the calculations and concepts involved. The discussion does not reach a consensus on all points raised.

Contextual Notes

There are unresolved mathematical steps and assumptions regarding the transformation of coordinates and the interpretation of simultaneity in different reference frames. The discussion highlights the complexity of applying the Lorentz transformation and understanding the invariance of the space-time interval.

Who May Find This Useful

This discussion may be useful for students and enthusiasts of physics, particularly those interested in special relativity, the Lorentz transformation, and the conceptual challenges associated with space-time intervals and simultaneity.

ersteller
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Hallo.
A question about the relationship between the formulas found using the Lorentz transform and the invariance of the space time interval.

Two events A and B occur at the same time and different space locations in system S, where A and B are at rest and at distance x.
The system S' moves with velocity v with respect to S.

I want to find the time interval t' that S' measures between A and B.

1. By using the Lorentz transform one finds immediately:

t' = -\gamma\frac{v}{c^{2}}x

2. By using the invariance of the space time interval:

{(ct')^{2} - x'^{2} = - x^{2}}

and using the contacted x' = \frac{x}{\gamma}

one finds (neglecting the negative square...)

t' = -\frac{v}{c^{2}}x

So here the gamma is missing... Must I understand that:

a.
With the Lorentz transform I find the value of the time interval 'assigned' at S' as measured by S (with the time dilation due to the relative velocity between S and S')

and

b.
With the invariance of the space time interval I find this time interval as measured by S' (analogously to the use of the contracted x' in the expression of the interval)?

Have I right understood?
Thank you
er
 
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I don't quite understand the wording of your question at the end, but think I can see where the anomaly in your calculation comes from. (NOTE: I'll use units where c = 1 to make the equations simpler; c can be replaced afterwards, using dimensional analysis.)

If we use the Lorentz transformation, setting t = 0,

t'=\gamma(t-vx)=-\gamma v x

just as you found. So far so good... And, again setting t = 0,

x'=\gamma(x-vt)=\gamma x

x^2=(x')^2-(t')^2

(t')^2=(x')^2-(x')^2\gamma^{-2}=(x')^2(1-(1-v^2))

(t')^2=v^2(x')^2=\gamma^2 v^2 x^2

(t')=\pm \gamma x v

You got inconsistent results because you put x and (x')^2 the wrong way round in the equation after you wrote "and using the contacted".
 
Thank you; have you please the patience to help me again?

My aim is to find t' using the invariance of the space time interval.
This interval calculated in S is x2.
This interval in S' should be x'2 - t'2.
It should be x'2 - t'2 = x2.

S' moves wrt S at velocity v, so, as I qualitatively understand, it should be x'<x.

You obtained the right result by putting x&#039; = \gamma x &gt; x.

I think I have here a HUGE misunderstanding :eek:!

Can you or somebody else please help me?
Thanks!
er
 
This is a common misconception. I had the same problem when I first learned it. You are thinking that x' should be less than x, because of length contraction. This is incorrect. In fact, for the case you stated x' >x, as Rasalhague showed. But then what about length contraction? How does that work? To understand this, you need to understand that events that are simultaneous in one frame are not necessarily simultaneous in the other frame. So, consider a rod of length L in the unprimed frame. The two ends of the bar have the following unprimed coordinates ( all coordinates are (t,x)):

E1 = (0,0) E2 = (0,L)

So in the unprimed frame, the length of the bar is the difference of the two x-coordinates, which is L. Now, transform these into primed coordinates using the Lorentz transformation, and you find:

E1&#039; = (0,0) E2&#039; = ({\beta} {\gamma} L, {\gamma} L)

Now, the length of the bar in the primed frame is not just the difference in the x coordinates, because the two events are now at different times . To find the length of the bar in the primed frame, I need to find coordinates of the two ends at the same value of t'. You can do this by asking what time in the unprimed frame gives a value of t' = 0 in the primed frame. These new events will be:

E1= (0,0) E3 = (-\beta L,L) E1&#039; = (0,0) E3&#039; = (0,\gamma (1-\beta^2)L) = (0,\frac{L}{\gamma})

Now we can find the length of the bar in the primed frame by just taking the difference of the x-coordinates between E1' and E3', which are now at the same time in the primed frame. As expected, now L'<L, indicating length contraction. Does this help?
 
Thank you phyzguy, it helps a lot!

Now I've understood my mistake and I can go on, and find other mistakes... :smile:

For example, from

<br /> {(ct&#039;)^{2} - x&#039;^{2} = - x^{2}}<br />

can one really find t' without using the Lorentz transformations? I thought yes, but how to?

Ciao e grazie
er
 
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